Abstract
Se80Ge20−x Cd x (0 ≤ x ≤ 12 at.%) compositions were prepared by the conventional melt quenching technique. Thin films with different thicknesses (200–620 nm) were deposited by thermal evaporation technique. Energy dispersive x-ray spectroscopy technique showed that the films are nearly stoichiometric. X-ray diffraction (XRD) patterns indicate that the films are in amorphous state. The DC conductivity and switching properties were investigated in the temperature range (293–393 K) below the corresponding glass transition temperature. The obtained results of DC conductivity showed that it increases with increasing Cd content in the considered system as well as with film thickness through the studied range of thickness. The conduction activation energy has two values, ΔE σ1 and ΔE σ2, indicating the presence of two different conduction mechanisms through the studied range of temperature. The obtained results of the temperature dependence of DC conductivity are explained in accordance with the Mott and Davis model for electrical conduction. The current–voltage (I–V) characteristic curves were studied for the investigated samples and found to be typical for a memory switch. The mean value of the threshold voltage \(\overline{{V}}_{\rm{th}}\) was found to increase linearly with film thickness and decrease exponentially with temperature in the investigated ranges of thickness and temperature. The threshold voltage activation energy ε th for the investigated samples was calculated from the corresponding temperature dependence of \(\overline{{V}}_{\rm{th}}\). The switching phenomenon observed in these films is explained in accordance with the electrothermal effect initiated by Joule heating for the switching process. The effect of Cd content on the studied parameters was also investigated.
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References
N. Yoshida, M. Itioh, and K. Tanaka, J. Non-Cryst. Solut. 198, 749 (1996).
N. Yamada, MRS Bull. 21, 48 (1996).
S.R. Ovshinsky, Phys. Rev. Lett. 21, 1450 (1968).
R. Landauer and J.W.F. Woo, Comments Solid State Phys. 4, 139 (1972).
D. Adler, M.S. Shur, M. Silver, and S.R. Ovshinsky, J. Appl. Phys. 51, 3289 (1980).
D. Adler, Sci. Am. 36, 236 (1977).
H. Fritzsche and S.R. Ovshinsky, J. Non-Cryst. Solids 4, 464 (1970).
R.M. Mehra, R. Shyan, and P.C. Mathur, J. Non-Cryst. Solids 31, 435 (1979).
A. Tolansky, Introduction to interferometry (New York: Longman, 1948), p. 148.
M.A. Afifi and N.A. Hegab, Vacuum 48, 135 (1997).
L.J. Pauling, Nature of Chemical Bond (New York: Cornell University Press, 1960), p. 88.
R.T. Sanderson, J. Am. Chem. Soc. 105, 2259 (1983).
M. Yamaguchi, Philos. Mag. B 51, 651 (1985).
A. Giridhar, P.C.L. Narasimham, and Sudna Mahadeven, J. Non-Cryst. Solids 43, 29 (1983).
N.F. Mott and E.A. Davis, Electronic Processes in Non-crystalline Materials (Oxford: Oxford University Press, 1979), p.377.
N.F. Mott and E.A. Davis, Philos. Mag. 22, 903 (1970).
J.C. Phillips, J. Non-Cryst. Solids 43, 37 (1981).
V. Kokorina, eds., Glasses for Infrared Optics (Boca Raton, FL: CRC, 1996), p. P29.
M.A. Afifi, N.A. Hegab, H.E. Atyia, and A.S. Farid, J. Alloys Compd. 463, 10 (2008).
J. Bicerano and S.R. Ovshinsky, J. Non-Cryst. Solids 74, 75 (1985).
M.A. Afifi, N.A. Hegab, H.E. Atyia, and M.I. Ismael, Vacuum 83, 326 (2008).
S. Abou El-Hassan and H. Khadar, Phys. Status Solidi a 186, 401 (2001).
A.H. Abou El-Ela, N. Abdelmohsen, and H.H. Labib, Appl. Phys. A 26, 171 (1981).
H.J. De Wit and C. Crevecoeur, Solid State Electron. 15, 729 (1972).
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Afifi, M., Hegab, N., Shakra, A. et al. Electrical and Switching Phenomenon of Se80Ge20−x Cd x (0 ≤ x ≤ 12 at.%) Amorphous System. J. Electron. Mater. 44, 87–95 (2015). https://doi.org/10.1007/s11664-014-3404-y
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DOI: https://doi.org/10.1007/s11664-014-3404-y